As we show
in [1]}, [2]}, the
Liouville operator for this class of CRNs takes the compact form
\(- \mathcal {L} \! \left( a^{\dagger } , a \right) ={\psi }^T_Y \! \left( a^{\dagger } \right){\mathbb {A}}_{\kappa } \,{\psi }_Y \! \left( a \right)\) 
